CN102798512B - Three-dimensional flow field image measurement device and method adopting single lens - Google Patents
Three-dimensional flow field image measurement device and method adopting single lens Download PDFInfo
- Publication number
- CN102798512B CN102798512B CN201210208458.7A CN201210208458A CN102798512B CN 102798512 B CN102798512 B CN 102798512B CN 201210208458 A CN201210208458 A CN 201210208458A CN 102798512 B CN102798512 B CN 102798512B
- Authority
- CN
- China
- Prior art keywords
- flow field
- particle
- dimensional
- imageing sensor
- amici prism
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Fee Related
Links
Landscapes
- Length Measuring Devices By Optical Means (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
Abstract
The invention discloses a three-dimensional flow field image measurement device and method adopting a single lens, which are characterized in that a polarized light source is used for illuminating a flow field to be detected; light from a camera lens is divided into two paths through a light splitting prism and polaroids are respectively used for carrying out polarization detection for the two paths; two CCDs (Charge Coupled Device) or CMOS (Complementary Metal-Oxide-Semiconductor Transistor) image sensors are respectively used for imaging; a relative gray level of a corresponding tracer particle in two pictures can be used for judging whether the tracer particle is located in front of a focusing plane or in back of the focusing plane; the distance between the position of the tracer particle and the focusing plane is computed according to the size of a defocusing amount of the tracer particle of the single picture, so as to only determine a three-dimensional position of the tracer particle; and a movement fuzzy parameter is combined to further obtain a three-dimensional movement speed of the tracer particle, namely the information of a three-dimensional flow field is obtained. The three-dimensional flow field image measurement device and method adopting the single lens have the beneficial effects that the three-dimensional measurement of a transient flow field can be realized by only one camera lens, a measurement system and a data processing process are simplified, and the system cost is reduced.
Description
technical field
The present invention relates to a kind of image measuring apparatus method of three-dimensional flow field, particularly a kind of based on fuzzy image processing, adopt the single-lens device and method that obtains three-dimensional flow field information.
Background technology
Along with the development of digital camera and computer technology, adopt digital camera to take trace particle and be used widely with the flow field survey instrument that obtains information of flow in recent years.For obtaining of three-dimensional flow field information, conventionally adopt two covers or overlap camera system more, carry out imaging from two or more visual angles.Two covers or overlap between camera system more and exist synchronous problem, adjust very difficult, data processing complex; And for shooting particle transient images or interference image clearly, conventionally require the time shutter extremely short, need configuration high-speed photographic apparatus and high energy pulse LASER Light Source etc., system cost is high.
Summary of the invention
The object of the invention is to develop a kind of based on fuzzy image processing, use the apparatus and method of single-lens measurement three-dimensional flow field, have advantages of that device is simple, easy and simple to handle, with low cost.
Ultimate principle of the present invention: at present conventional image method flow field survey process, on the one hand, for fear of because trace particle motion causes image quality decrease, all require the time shutter extremely short; But from another angle, if the proper extension time shutter, the athletic meeting of interior trace particle at this moment forms fuzzy movement locus image, and this blurring trajectorie image has comprised the movable information of trace particle, i.e. velocity field information.On the other hand, for preventing that defocus blur from causing interference to measurement result, general measuring method all adopts very thin laser light sheet to throw light on to field depth inner region, make illuminated trace particle can be on the focal plane of camera blur-free imaging; But from another angle, in fact the out of focus phenomenon of image has comprised the information of trace particle with focusing plane distance, further trace particle is positioned at before or after focal plane and is judged, in conjunction with the planimetric coordinates of two dimensional image, can obtain trace particle three dimensional local information accurately.Comprehensive above-mentioned 2 can obtain three-dimensional flow field information accurately.
Based on above-mentioned inventive principle, technical scheme of the present invention is: a kind ofly adopt single-lens three-dimensional flow field image measuring apparatus, be characterized in, device is by polarized light source, camera lens, Amici prism, the first polaroid, the second polaroid, the first imageing sensor, the second imageing sensor and computing machine composition, described polarized light source is placed on flow field to be measured or by the form flow field to be measured of throwing light on, described Amici prism is placed in after camera lens, the incident surface A of described Amici prism is relative with camera lens, a side difference aplanatism of Amici prism exit facet B and exit facet C is apart from the first imageing sensor and the second imageing sensor that arrange, the first described polaroid, the second polaroid is separately positioned on the centre of Amici prism the second exit facet C and the first imageing sensor, the first exit facet B of Amici prism and the centre of the second imageing sensor.Amici prism can be the Amici prism of semi-transparent semi-reflecting prism, five jiaos of Amici prisms or other form.
The first described polaroid and the second polaroid can form an entirety on 2 surfaces of Amici prism the first exit facet B and the second exit facet C by plated film mode plated film, or Amici prism, the first polaroid and the second polaroid are replaced by a polarization splitting prism.
Described Amici prism can be replaced by 1 semi-transparent semi-reflecting plane beam splitter.
Described camera lens is telecentric lens or non-telecentric lens, and described the first imageing sensor, the second imageing sensor are selected CCD or cmos device.
A three-dimensional flow field image measuring method that adopts above-mentioned single-lens three-dimensional flow field image measuring apparatus, is characterized in, measuring method step is:
1. before measuring, first adopt transparent calibrated thing to demarcate to measurement mechanism, obtain the physical size of pixel (pixel) representative;
2. adopt the polarized light source flow field to be measured of throwing light on, regulate position and the intensity size of polarized light source, and adjust polarization angle, make bias light even;
3. Amici prism is placed in after camera lens, received light source is divided into two-way by Amici prism, adopt orthogonal the first polaroid of polarization angle and the second polaroid to carry out after analyzing to two-way light, adopt respectively the first imageing sensor and the second imageing sensor imaging of CCD or CMOS, because two imageing sensors are identical with the optical path length between camera lens, ensure that the visual field photographing is identical;
4. regulate the camera exposure time, the situation of the coincidence of trace particle track and adhesion in the imaging of minimizing imageing sensor, and treat the trace particle of surveying in flow field regions and take, by the image input computing machine obtaining;
5. on computers first gathered image is carried out to denoising, secondly judge the defocusing amount of image by image fog edge scale graded, consider that two width picture visual fields corresponding to different polarization direction are identical, can judge that by the relative gray scale of corresponding trace particle in this two width picture trace particle is positioned at before focal plane or to behind focal plane, thereby set up the corresponding relation of fuzzy yardstick δ and defocusing amount Δ W, as shown in Equation 1
(1)
In formula,
r 'for the fuzzy image radius of out of focus particle, Δ W is that actual object plane departs from the distance to focal plane, is obtained by camera parameter
wobject distance during for accurate focusing, δ is the poor of the blurred picture radius R ' of out of focus particle and the blurred picture particle radii that radially 2 edge gradient maximum amplitudes calculate; Blurred picture gradient magnitude can calculate from following formula:
(2)
In formula
f (x, y)it is the coordinate function of trace particle image pixel;
Because the two width picture visual fields that different polarization direction is corresponding are identical, can judge that by the relative gray scale of corresponding trace particle in this two width picture trace particle is positioned at before focal plane or to behind focal plane, three-dimensional position that thus can unique definite trace particle; Within the time shutter, in the time that there is displacement on particle edge perpendicular to camera plane direction, can judge along the defocusing amount of direction of motion and change by said method, in conjunction with movement of particles blurring trajectorie length on imaging plane, obtain particle three-dimensional motion direction and actual motion course length
l, the known camera exposure time
t, can obtain the three-dimensional motion speed of trace particle by following formula
v:
(3)
Obtained three-dimensional flow field information by the processing of blurred picture thus.
The invention has the beneficial effects as follows the three-dimensional measurement that only just can realize flow field with a camera lens, instead of two or more cameras are taken the trace particle in flow field to be measured from different perspectives, or a camera fast moving is to take the trace particle in flow field to be measured, not only avoid two cover or the synchronous problems of many cover systems, and simplified measuring system and data handling procedure, reduced system cost.
Brief description of the drawings
Fig. 1 is the embodiment of the present invention 1 schematic diagram;
Fig. 2 is the embodiment of the present invention 2 schematic diagram;
Fig. 3 is the embodiment of the present invention 3 schematic diagram.
Fig. 4 is the embodiment of the present invention 4 schematic diagram;
Fig. 5 is the embodiment of the present invention 5 schematic diagram.
embodiment
A kind ofly adopt single-lens three-dimensional flow field image measuring apparatus embodiment 1, as shown in Figure 1, be characterized in, device is by polarized light source 1, camera lens 2, Amici prism 3, the first polaroid 4, the second polaroid 5, the first imageing sensor 6, the second imageing sensor 7 and computing machine 8 form, described polarized light source 1 is placed on flow field to be measured by the form flow field of throwing light on, described Amici prism 3 is placed in after camera lens 2, the incident surface A of described Amici prism 3 is relative with camera lens 2, a side difference aplanatism of Amici prism 3 first exit facet B and the second exit facet C is apart from the second imageing sensor 6 and the first imageing sensor 7 that arrange, the first described polaroid 4, the second polaroid 5 is separately positioned on the centre of Amici prism 3 second exit facet C and the first imageing sensor 6, the first exit facet B of Amici prism 3 and the centre of the second imageing sensor 7.
A kind of step of the three-dimensional flow field image measuring method that adopts above-mentioned single-lens three-dimensional flow field image measuring apparatus is:
1. before measuring, first measurement mechanism is demarcated; If micro-scale is as measuring object, obtain the physical size of focal length measurement hypograph sensor 6 and 7 unit picture element representatives using transparent calibrated thing;
2. adopt polarized light source 1 flow field to be measured of throwing light on, regulate position and the intensity size of polarized light source 1, and adjust polarization angle, make bias light even;
3. Amici prism 3 is placed in after camera lens 2, received light source is divided into two-way by Amici prism 3, adopt orthogonal the first polaroid 4 of polarization angle and the second polaroid 5 to carry out after analyzing to two-way light, adopt respectively the first imageing sensor 6 and the second imageing sensor 7 imagings of CCD or CMOS, because two imageing sensors are identical with the optical path length of camera lens 2, ensure that the visual field photographing is identical;
4. regulate the camera exposure time, the situation of the coincidence of trace particle track and adhesion in the imaging of minimizing imageing sensor, and treat the trace particle of surveying in flow field regions and take, by the image input computing machine obtaining;
5. on computing machine 8, first gathered image is carried out to denoising, secondly judge the defocusing amount of image by image fog edge scale graded, consider that two width picture visual fields corresponding to different polarization direction are identical, can judge that by the relative gray scale of corresponding trace particle in this two width picture trace particle is positioned at before focal plane or to behind focal plane, thereby set up the corresponding relation of fuzzy yardstick δ and defocusing amount Δ W, as shown in Equation 1
(1)
In formula,
r 'for the fuzzy image radius of out of focus particle, Δ W is that actual object plane departs from the distance to focal plane, is obtained by camera parameter
wobject distance during for accurate focusing, δ is the poor of the blurred picture radius R ' of out of focus particle and the blurred picture particle radii that radially 2 edge gradient maximum amplitudes calculate;
Blurred picture gradient magnitude can calculate from following formula:
(2)
In formula
f (x, y)it is the coordinate function of trace particle image pixel;
Because the two width picture visual fields that different polarization direction is corresponding are identical, can judge that by the relative gray scale of corresponding trace particle in this two width picture trace particle is positioned at before focal plane or to behind focal plane, three-dimensional position that thus can unique definite trace particle; Within the time shutter, in the time that there is displacement on particle edge perpendicular to camera plane direction, can judge along the defocusing amount of direction of motion and change by said method, in conjunction with movement of particles blurring trajectorie length on imaging plane, obtain particle three-dimensional motion direction and actual motion course length
l, the known camera exposure time
t, can obtain the three-dimensional motion speed of trace particle by following formula
v:
(3)
Obtained three-dimensional flow field information by the processing of blurred picture thus.
Embodiment 2:
As the first polaroid 4 in embodiment 1 and the second polaroid 5 being plated in to 2 surfaces of Amici prism the second exit facet C and the first exit facet B in plated film mode, as shown in Figure 2, in aggregates by the Amici prism 3 in embodiment 1, the first polaroid 4 and the second polaroid 5 structures, measuring process is identical with embodiment 1 operating process.
Embodiment 3:
As shown in Figure 3, also the Amici prism in embodiment 13, the first polaroid 4 and the second polaroid 5 use polarization splitting prisms 9 can be replaced, 7 of the first imageing sensor 6 and the second imageing sensors are placed in respectively two exit facet one sides of polarization splitting prism 9 with aplanatism distance, measuring process is identical with embodiment 1 operating process.
Embodiment 4:
As shown in Fig. 4, also the 3 use plane beam splitters 10 of the Amici prism in embodiment 1 can be replaced, this plane beam splitter 10 is on optics plain film, to plate spectro-film to form.
Embodiment 5:
As shown in Figure 5, camera lens 2 adopts telecentric lens 11, and in the field depth of telecentric lens, object image size does not change with the variation of position, can obtain like this size of trace particle or other particle.Measuring process is also identical with embodiment 1 operating process.
In five above-mentioned embodiment, the first imageing sensor, the second imageing sensor are all selected CCD or cmos device.In 1,2,3,4 above-mentioned embodiment, camera lens 2 is non-telecentric lens, and in embodiment 5, camera lens 2 adopts telecentric lens, and camera lens numbering 2 is revised as to 11.
Claims (1)
1. one kind adopts the three-dimensional flow field image measuring method of single-lens three-dimensional flow field image measuring apparatus, described device is by polarized light source (1), camera lens (2), Amici prism (3), the first polaroid (4), the second polaroid (5), the first imageing sensor (6), the second imageing sensor (7) and computing machine (8) composition, described polarized light source (1) is placed on flow field to be measured, described Amici prism (3) is placed in after camera lens (2), the incident surface A of described Amici prism (3) is relative with camera lens (2), a side of Amici prism (3) second exit facet C and the first exit facet B respectively aplanatism distance arranges the first imageing sensor (6) and the second imageing sensor (7), described the first polaroid (4), the second polaroid (5) is separately positioned on the centre of the centre of Amici prism (3) second exit facet C and the first imageing sensor (6) and the first exit facet B of Amici prism (3) and the second imageing sensor (7), it is characterized in that, measuring method step is:
1) before measurement, first measurement mechanism is demarcated, adopted transparent calibrated thing, obtain the physical size of pixel representative;
2) adopt polarized light source (1) flow field to be measured of throwing light on, regulate position and the intensity size of polarized light source (1), and adjust polarization angle, make bias light even;
3) Amici prism (3) is placed in after camera lens (2), received light source is divided into two-way by Amici prism (3), adopt orthogonal the first polaroid of polarization angle (4) and the second polaroid (5) to carry out after analyzing to two-way light, adopt respectively the first imageing sensor (6) and the second imageing sensor (7) imaging of CCD or CMOS, because two imageing sensors are identical with the optical path length of camera lens (2), ensure that the visual field photographing is identical;
4) regulate the camera exposure time, in the imaging of minimizing imageing sensor, the situation of the coincidence of trace particle track and adhesion, treats the trace particle of surveying in flow field regions and takes, by the image input computing machine (8) obtaining;
5) above first gathered image is carried out to denoising at computing machine (8), secondly judge the defocusing amount of image by image fog edge scale graded, consider that two width picture visual fields corresponding to different polarization direction are identical, can judge that by the relative gray scale of corresponding trace particle in this two width picture trace particle is positioned at before focal plane or to behind focal plane, thereby set up the corresponding relation of fuzzy yardstick δ and defocusing amount Δ W, as shown in Equation 1
(1)
In formula,
r 'for the fuzzy image radius of out of focus particle, Δ W is that actual object plane departs from the distance to focal plane, is obtained by camera parameter
wobject distance during for accurate focusing, δ is the poor of the blurred picture radius R ' of out of focus particle and the blurred picture particle radii that radially 2 edge gradient maximum amplitudes calculate;
Blurred picture gradient magnitude can calculate from following formula:
(2)
In formula
f (x, y)it is the coordinate function of trace particle image pixel;
Because the two width picture visual fields that different polarization direction is corresponding are identical, can judge that by the relative gray scale of corresponding trace particle in this two width picture trace particle is positioned at before focal plane or to behind focal plane, three-dimensional position that thus can unique definite trace particle; Within the time shutter, in the time that there is displacement on particle edge perpendicular to camera plane direction, can judge along the defocusing amount of direction of motion and change by said method, in conjunction with movement of particles blurring trajectorie length on imaging plane, obtain particle three-dimensional motion direction and actual motion course length
l, the known camera exposure time
t, can obtain the three-dimensional motion speed of trace particle by following formula
v:
(3)
Obtained three-dimensional flow field information by the processing of blurred picture thus.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201210208458.7A CN102798512B (en) | 2012-06-25 | 2012-06-25 | Three-dimensional flow field image measurement device and method adopting single lens |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201210208458.7A CN102798512B (en) | 2012-06-25 | 2012-06-25 | Three-dimensional flow field image measurement device and method adopting single lens |
Publications (2)
Publication Number | Publication Date |
---|---|
CN102798512A CN102798512A (en) | 2012-11-28 |
CN102798512B true CN102798512B (en) | 2014-11-26 |
Family
ID=47197696
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201210208458.7A Expired - Fee Related CN102798512B (en) | 2012-06-25 | 2012-06-25 | Three-dimensional flow field image measurement device and method adopting single lens |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN102798512B (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN110410260A (en) * | 2019-07-29 | 2019-11-05 | 西华大学 | A kind of detection method of the flow field flow image of energy conversion device |
Families Citing this family (15)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN103209307B (en) * | 2013-04-18 | 2016-05-25 | 清华大学 | Coding refocusing is calculated image capture method and device |
CN104019763B (en) * | 2014-06-18 | 2016-11-23 | 重庆大学 | Fluid 3D velocity field and the synchronous measuring apparatus of deformable body three-dimensional appearance |
CN104316289A (en) * | 2014-10-20 | 2015-01-28 | 中国航天空气动力技术研究院 | High-supersonic velocity wind tunnel dual-optical path system |
CN104808012B (en) * | 2015-05-15 | 2018-07-27 | 北京航空航天大学 | A kind of three-dimensional velocity coupling pressure measurement method and system |
CN105043714A (en) * | 2015-07-09 | 2015-11-11 | 广东电网有限责任公司电力科学研究院 | Simulation test device and method of three-dimensional flow field in CFB boiler |
CN105424558B (en) * | 2015-11-03 | 2018-05-22 | 上海理工大学 | A kind of burning particles multiparameter measuring device and method using blue light back lighting |
CN105738648B (en) * | 2016-04-19 | 2018-08-10 | 中国科学院过程工程研究所 | The On-line Measuring Method of particle speed in a kind of heterogeneous system |
CN106153977A (en) * | 2016-06-21 | 2016-11-23 | 上海交通大学 | A kind of three-dimensional flow field method of testing based on single light-field camera |
CN107748055A (en) * | 2017-06-09 | 2018-03-02 | 珠江水利委员会珠江水利科学研究院 | Water surface flow field acquisition method |
CN107631857B (en) * | 2017-07-21 | 2020-04-07 | 哈尔滨工程大学 | System for measuring fine flow field between main body pieces of trimaran |
CN109580169B (en) * | 2018-12-27 | 2024-04-05 | 中国科学院西安光学精密机械研究所 | Binocular vision-based underwater vibrating table video measurement system |
CN111007278A (en) * | 2019-12-12 | 2020-04-14 | 中国空气动力研究与发展中心 | Acceleration measuring method and device based on particle image velocimetry and storage medium |
CN111007279A (en) * | 2019-12-12 | 2020-04-14 | 中国空气动力研究与发展中心 | Acceleration measuring device based on particle image velocimetry and polarization device |
CN113747142A (en) * | 2021-08-16 | 2021-12-03 | 合肥芯福传感器技术有限公司 | Passive single photon imaging 3D camera and shooting method |
CN116580076B (en) * | 2023-07-10 | 2023-09-12 | 中国空气动力研究与发展中心计算空气动力研究所 | Device, method, apparatus and medium for acquiring particle graph containing model boundary |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN2773689Y (en) * | 2004-08-18 | 2006-04-19 | 浙江大学 | Imaging micro-speed measuring device for micro-fluid particle |
CN101078765A (en) * | 2007-07-05 | 2007-11-28 | 北京航空航天大学 | Laser radar remote sensing polarized imaging system |
CN201322649Y (en) * | 2008-12-29 | 2009-10-07 | 浙江大学 | Full-polarization image measuring system |
Family Cites Families (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP4490061B2 (en) * | 2003-08-21 | 2010-06-23 | シスメックス株式会社 | Particle image analyzer |
JP2005140528A (en) * | 2003-11-04 | 2005-06-02 | Toshiba Corp | Fluid measurement device |
-
2012
- 2012-06-25 CN CN201210208458.7A patent/CN102798512B/en not_active Expired - Fee Related
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN2773689Y (en) * | 2004-08-18 | 2006-04-19 | 浙江大学 | Imaging micro-speed measuring device for micro-fluid particle |
CN101078765A (en) * | 2007-07-05 | 2007-11-28 | 北京航空航天大学 | Laser radar remote sensing polarized imaging system |
CN201322649Y (en) * | 2008-12-29 | 2009-10-07 | 浙江大学 | Full-polarization image measuring system |
Non-Patent Citations (3)
Title |
---|
D.Lebrun等.Methods for the deconvolution of defocused-image pairs recorded separately on two CCD cameras: application to particle sizing.《APPLIED OPTICS》.1996,第35卷(第32期),第6375-6376页. * |
JP特开2005-140528A 2005.06.02 * |
Methods for the deconvolution of defocused-image pairs recorded separately on two CCD cameras: application to particle sizing;D.Lebrun等;《APPLIED OPTICS》;19961110;第35卷(第32期);第6375-6376页 * |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN110410260A (en) * | 2019-07-29 | 2019-11-05 | 西华大学 | A kind of detection method of the flow field flow image of energy conversion device |
Also Published As
Publication number | Publication date |
---|---|
CN102798512A (en) | 2012-11-28 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN102798512B (en) | Three-dimensional flow field image measurement device and method adopting single lens | |
CN102692364B (en) | Blurring image processing-based dynamic grain measuring device and method | |
US7612870B2 (en) | Single-lens aperture-coded camera for three dimensional imaging in small volumes | |
CN102494609B (en) | Three-dimensional photographing process based on laser probe array and device utilizing same | |
US8339463B2 (en) | Camera lens calibration system | |
CN101825431B (en) | Reference image techniques for three-dimensional sensing | |
US20070189750A1 (en) | Method of and apparatus for simultaneously capturing and generating multiple blurred images | |
JP5873430B2 (en) | Imaging apparatus, imaging method, program, and integrated circuit | |
CN101183206A (en) | Method for calculating distance and actuate size of shot object | |
JPH01216306A (en) | Focus detecting device having image pickup means | |
CN111492201A (en) | Distance measuring camera | |
JP2013044844A (en) | Image processing device and image processing method | |
JPH11337313A (en) | Distance measuring device and method thereof, and image restoration device and method thereof | |
CN107024417A (en) | Three dimensional particles field measurement device and method based on single-lens multi-pass optical field imaging | |
CN108305547A (en) | A kind of system and method measuring grating constant | |
WO2024104502A1 (en) | Imaging method and system based on lens compensation | |
GB2510537A (en) | Observation device | |
CN106595516B (en) | A kind of big depth of field structural light measurement method based on tight shot | |
JP6376809B2 (en) | Projection device and imaging device used in three-dimensional shape measurement system | |
JP2001504592A (en) | Distance measuring method and distance measuring device | |
WO2014073590A1 (en) | Three-dimensional measuring device and three-dimensional measuring method | |
Heikkinen et al. | Perspective error reduction in 2D digital image correlation measurements by combination with defocused speckle imaging | |
KR101423829B1 (en) | 3D Shape Mesurement Mehod and Device by using Amplitude of Projection Grating | |
JP2012220349A (en) | Displacement and distortion distribution measurement optical system and measurement method | |
CN109470145A (en) | Polarization Modulation high resolution Stereo Vision Measurement System and method |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
C06 | Publication | ||
PB01 | Publication | ||
C10 | Entry into substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
C14 | Grant of patent or utility model | ||
GR01 | Patent grant | ||
CF01 | Termination of patent right due to non-payment of annual fee | ||
CF01 | Termination of patent right due to non-payment of annual fee |
Granted publication date: 20141126 Termination date: 20180625 |